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#1
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Owen Duffy wrote:
I say that the phase relation MUST be the same everywhere on the coil. That does not seem to me to support Cecil's proposition at all, I understand Cecil to argue that there is a substantial phase change in the coil current along the coil. Please understand exactly what I am saying, Owen. 1. There is a *substantial* phase change in the *traveling-wave* current along the coil. Traveling-wave current is hard to measure in a standing-wave antenna but its phase yields complete and accurate phase/delay information. 2. There is virtually *no* phase change in the *standing-wave* current along the coil. Standing-wave current is easy to measure in a standing-wave antenna but its phase yields close to *zero phase/delay information*. 3. In a standing-wave antenna, the total current is primarily standing-wave current. In a loaded mobile antenna, the standing- wave current is approximately 90% of the total current thus tending to mask the traveling-wave current. W8JI's and W7EL's "measurements" were made using standing- wave current. They should have instead used traveling-wave current. It's an easy mistake to make but one would think, after five years, it is time to admit the mistake. -- 73, Cecil http://www.w5dxp.com |
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#2
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Cecil Moore wrote: Please understand exactly what I am saying, Owen. 1. There is a *substantial* phase change in the *traveling-wave* current along the coil. Traveling-wave current is hard to measure in a standing-wave antenna but its phase yields complete and accurate phase/delay information. 2. There is virtually *no* phase change in the *standing-wave* current along the coil. Standing-wave current is easy to measure in a standing-wave antenna but its phase yields close to *zero phase/delay information*. 3. In a standing-wave antenna, the total current is primarily standing-wave current. In a loaded mobile antenna, the standing- wave current is approximately 90% of the total current thus tending to mask the traveling-wave current. Honestly, Cecil, it's pretty hard to know what you mean considering the reckless way you throw around the term 'phase'. I'll grant that you might know what you mean, but I don't see how you can expect anyone else to. 73, ac6xg |
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#3
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Jim Kelley wrote:
Honestly, Cecil, it's pretty hard to know what you mean considering the reckless way you throw around the term 'phase'. I'll grant that you might know what you mean, but I don't see how you can expect anyone else to. Jim, if you have trouble understanding the word "phase", look it up in a technical dictionary. I don't have time to waste my time teaching everyone the principles of AC waves in EE201. But assuming some others are having the same problem as you: From the IEEE Dictionary: "phase - The fractional part t/P of the period P through which t has advanced relative to an arbitrary origin." FYI: For a signal proportional to cos(x)*cos(wt), the phase doesn't change with 'x'. That's why standing wave current cannot be used to measure delay. -- 73, Cecil http://www.w5dxp.com |
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#4
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Cecil Moore wrote: Jim Kelley wrote: Honestly, Cecil, it's pretty hard to know what you mean considering the reckless way you throw around the term 'phase'. I'll grant that you might know what you mean, but I don't see how you can expect anyone else to. Jim, if you have trouble understanding the word "phase", look it up in a technical dictionary. I don't have time to waste my time teaching everyone the principles of AC waves in EE201. Thanks. Sorry for the unfinished thought. I meant that because of the reckless way you use the term, I don't know how you expect others to know what you intend by it when you use it. FYI: For a signal proportional to cos(x)*cos(wt), the phase doesn't change with 'x'. That's why standing wave current cannot be used to measure delay. Perfect example. The phase of a cosine wave at it's absolute maximum amplitude is either 0 or 180 degrees. Each point along a sinusoidal plot represents a different phase angle. Phase varies with time at a fixed position, or varies with position at a fixed time. For it to have meaning there must be a reference. You have a habit of switching references without noticing or making note of it. This makes some of your comments a bit confused sounding, if not blatantly inaccurate. With regard to your comment above, if the maximum amplitude and period of a sinusoidal wave are both known, then given any instantaneous amplitude and, knowing whether the slope is positive or negative, the instantaneous phase can be readily determined. FYI: Phase angle (wt) is found on the x axis of a sinusoidal plot. When period or wavelength and length are equated, as is the case with a resonant antenna then phase and position are functionally related. 73, ac6xg |
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#5
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Jim Kelley wrote:
You have a habit of switching references without noticing or making note of it. This makes some of your comments a bit confused sounding, if not blatantly inaccurate. Jim, it's all your fault for not being telepathic. :-) I admit that my thought processes are somewhat chaotic but remember, order often comes out of chaos. I've experienced an epiphany or two in my time. I also have a bad habit of declaring something invalid when it is only irrelevant. It is the conclusions drawn from irrelevant measurements that are invalid, not the measurements themselves. The convention that I try to use is the EZNEC convention. Everything is referenced to the source signal. When I say the phase of a standing wave is unchanging, I mean that it has the same phase as the source signal at the feedpoint and is the same phase as reported by EZNEC. I apologize for not being clear about that. With regard to your comment above, if the maximum amplitude and period of a sinusoidal wave are both known, then given any instantaneous amplitude and, knowing whether the slope is positive or negative, the instantaneous phase can be readily determined. Take I = K1*cos(x)*cos(wt), a standing-wave equation. Let t be any fixed value. cos(x) is an amplitude value and does NOT vary with time. Therefore, the phase of the standing-wave signal is constant at any particular time and does NOT depend upon position along the wire or coil. Now take I = K2*cos(x+wt), a traveling-wave equation. Let t be any fixed value. The length dimension 'x' has an effect on phase, i.e. the phase of of the signal indeed does depend upon BOTH position AND time. Anyone who understands the math would not dare show his ignorance by asserting that the delay through a 100T coil is 3 ns on 4 MHz or that the measured phase shift through a loading coil is somehow proportional to the delay through the coil in a standing-wave antenna. -- 73, Cecil http://www.w5dxp.com |
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#6
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Cecil Moore wrote:
With regard to your comment above, if the maximum amplitude and period of a sinusoidal wave are both known, then given any instantaneous amplitude and, knowing whether the slope is positive or negative, the instantaneous phase can be readily determined. Take I = K1*cos(x)*cos(wt), a standing-wave equation. Let t be any fixed value. cos(x) is an amplitude value and does NOT vary with time. Therefore, the phase of the standing-wave signal is constant at any particular time and does NOT depend upon position along the wire or coil. The item residing inside the parentheses of a sinusoidal function is in fact the 'phase' of that function. In the expression above, at any given time, amplitude is determined by the independent variable, position. Accordingly, for any given position and time there is a unique amplitude and phase. Anyone who understands the math would not dare show his ignorance by asserting that the delay through a 100T coil is 3 ns on 4 MHz or that the measured phase shift through a loading coil is somehow proportional to the delay through the coil in a standing-wave antenna. In the face of such a redoubtable accusation I'm somewhat reluctant to admit my view that a phase shift across a coil of this sort would in fact be directly proportional to any propagation delay through that coil. 73, ac6xg |
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#7
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Jim Kelley wrote:
In the face of such a redoubtable accusation I'm somewhat reluctant to admit my view that a phase shift across a coil of this sort would in fact be directly proportional to any propagation delay through that coil. That's certainly true for traveling-wave current. Definitely not true for standing-wave current which doesn't change phase. I don't know that the comprehension problem is here - maybe this graph will help. http://www.w5dxp.com/travstnd.gif -- 73, Cecil http://www.w5dxp.com |
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#8
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Cecil Moore wrote:
Take I = K1*cos(x)*cos(wt), a standing-wave equation. Let t be any fixed value. cos(x) is an amplitude value and does NOT vary with time. Therefore, the phase of the standing-wave signal is constant at any particular time and does NOT depend upon position along the wire or coil. Now take I = K2*cos(x+wt), a traveling-wave equation. Let t be any fixed value. The length dimension 'x' has an effect on phase, i.e. the phase of of the signal indeed does depend upon BOTH position AND time. Cecil, I know what you are trying to say, but you got the message screwed up. If 't' is fixed, then the equations are essentially the same with regard to 'x'. That is typical; a snapshot in time does not say much about the wave behavior. 73, Gene W4SZ |
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#9
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Gene Fuller wrote:
Cecil Moore wrote: Take I = K1*cos(x)*cos(wt), a standing-wave equation. Let t be any fixed value. cos(x) is an amplitude value and does NOT vary with time. Therefore, the phase of the standing-wave signal is constant at any particular time and does NOT depend upon position along the wire or coil. Now take I = K2*cos(x+wt), a traveling-wave equation. Let t be any fixed value. The length dimension 'x' has an effect on phase, i.e. the phase of of the signal indeed does depend upon BOTH position AND time. Cecil, I know what you are trying to say, but you got the message screwed up. If 't' is fixed, then the equations are essentially the same with regard to 'x'. That is typical; a snapshot in time does not say much about the wave behavior. 73, Gene W4SZ It's generally cos(kx), but maybe Cecil is using a wave where k = 1, that is, the wavelength is 2*Pi. 73, Tom Donaly, KA6RUH |
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#10
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Jim Kelley wrote:
Cecil Moore wrote: Jim Kelley wrote: Honestly, Cecil, it's pretty hard to know what you mean considering the reckless way you throw around the term 'phase'. I'll grant that you might know what you mean, but I don't see how you can expect anyone else to. Jim, if you have trouble understanding the word "phase", look it up in a technical dictionary. I don't have time to waste my time teaching everyone the principles of AC waves in EE201. Thanks. Sorry for the unfinished thought. I meant that because of the reckless way you use the term, I don't know how you expect others to know what you intend by it when you use it. FYI: For a signal proportional to cos(x)*cos(wt), the phase doesn't change with 'x'. That's why standing wave current cannot be used to measure delay. Perfect example. The phase of a cosine wave at it's absolute maximum amplitude is either 0 or 180 degrees. Each point along a sinusoidal plot represents a different phase angle. Phase varies with time at a fixed position, or varies with position at a fixed time. For it to have meaning there must be a reference. You have a habit of switching references without noticing or making note of it. This makes some of your comments a bit confused sounding, if not blatantly inaccurate. With regard to your comment above, if the maximum amplitude and period of a sinusoidal wave are both known, then given any instantaneous amplitude and, knowing whether the slope is positive or negative, the instantaneous phase can be readily determined. FYI: Phase angle (wt) is found on the x axis of a sinusoidal plot. When period or wavelength and length are equated, as is the case with a resonant antenna then phase and position are functionally related. 73, ac6xg It's hardly surprising that Cecil thinks there's no phase information in a standing wave, since he leaves it out on purpose. "Cos(x)*Cos(wt)" is just flat wrong. It's supposed to be "Cos(x + d/2)*e^(i(wt + d/2))." "d" is the phase difference between a wave traveling in the forward direction and an equal amplitude wave traveling in the opposite direction. This is pretty poor shooting for a guy who claims a degree in symbol slinging. 73, Tom Donaly, KA6RUH |
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